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中国物理学会期刊

横向矩形微槽抑制高超声速第二模态扰动波的参数化研究

CSTR: 32037.14.aps.71.20220851

Parametrization of suppressing hypersonic second-mode waves by transverse rectangular microgrooves

CSTR: 32037.14.aps.71.20220851
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  • 针对高超声速飞行器边界层转捩控制问题, 以马赫数6平板边界层的第二模态扰动波为研究对象, 采用线性稳定性理论(LST)和直接数值模拟(DNS)分别开展了离散模态的同步模式研究和大尺寸(0.4 mm宽)横向矩形微槽开槽位置对第二模态扰动波的控制作用研究. LST分析表明: 涡/熵波会导致Mack第二模态和“mode I”模态(通常来源于快声波)的分支类型发生改变. 通过DNS发现, 开槽表面对基本流的影响程度与边界层流向位置(或厚度)相关, 随着开槽位置后移(边界层厚度增加), 开槽表面对基本流动的影响程度减弱, 摩擦阻力系数和压差阻力系数也逐渐减小. DNS结果还表明, 位于快/慢模态同步区间之前的开槽工况对第二模态扰动波依然有抑制效果, 这与文献中关于小尺寸(微米量级)微孔隙位置对第二模态控制作用的结论不同, 同时发现, 当矩形微槽布置在最大增长率区间范围内或快/慢模态同步区间位置时, 对第二模态扰动的抑制效果最佳.

     

    Aiming at delaying boundary-layer transition of hypersonic vehicles, the second-mode wave in the boundary layer of a Mach 6 flat plate is studied. Linear stability theory (LST) and direct numerical simulations (DNS) are used to investigate the discrete modes and the relation between the suppressing effect of second-mode wave and the location of transverse rectangular micro-groove (0.4 mm in width), respectively. The LST results show that vortex/entropy waves cause the branch types of Mack’s second mode and “mode I” modes (usually derived from fast acoustic waves) to change. The DNS results show that the influence of the grooved surface on the base flow depends on the streamwise location (or boundary-layer thickness). As the grooved surface shifts backward (or thickness increases), the influence of intensity on the base flow decreases, and the friction resistance coefficient Cd_\textf , differential pressure resistance coefficient Cd_\textp and total resistance coefficient Cd_x of the grooved surface also decrease. It is found that the grooves located in front of the synchronization region of the fast mode and slow mode still have an inhibitory effect on the second-mode wave, which is different from the effect of small-sized (micrometer scale) micro-pores reported in the literature. It is also found that the suppression effect on the second-mode wave is best when the grooves are arranged in the vicinity of the maximum growth-rate point or at the location of the synchronization interval of the fast mode and slow mode.

     

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